| 5073029 | Multisource device for photometric analysis and associated chromogens | December, 1991 | Eberly et al. | 356/436 |
| EP0062160 | March, 1982 | Method for the transillumination of fluid samples in containers. | ||
| JP5544969 | March, 1980 | 356/319 | ||
| GB1192008 | May, 1970 | |||
| GB1340811 | December, 1973 |
The invention relates to photometers where the amount of light passing through cuvettes arranged in a row is measured. In particular the invention relates to the distribution of light in the cuvettes.
In the prior art there are known photometers, particularly designed to be used in clinical analyses, where the samples under measurement are placed in a matrix-form cuvette assembly comprising 8×12 cuvettes, which is made of transparent plastic throughout. The absorbence is measured row by row, so that from a common light source, light is conducted via separate light paths to each cuvette, and further to respective detectors.
A problem in the above described apparatuses is that the light emissions passing through adjacent channels disturb each other in the measurement.
The main object of the present invention is to solve the said problem. This is achieved by means of the methods described in the appended patent claims.
In the drawings of the specification, FIG. 1 illustrates an arrangement for conducting light through the cuvette assembly using a movable light-cutting surface, e.g., a cylinder, and FIG. 2 illustrates a light distribution light-cutting disc or plate to be employed in the arrangement .
The arrangement of the drawings is carried out in an 8-channel photometer, where the employed cuvette assembly can be a regular 8×12 microtitration plate. When carrying out the measurement, a row 1 of eight cuvettes is brought to the measuring position, where light is conducted by means of light fibers 2, through lower lenses 3, to each cuvette from below. Above the cuvettes, the light that has passed through each cuvette is collected, by means of upper lenses 4, to detectors 5. The first ends of the fibers 2 are collected by an input collar 6 to form a beam of rays, whereto the emission from the light source is conducted. From each fiber, the light passes through a collar 7 vertically upwards to each cuvette.
The outlet collars 7 of the fibers 2 are located inside a horizontal cylinder 8, which is open at one end. The cylinder is made of some material impermeable to light. The cylinder is rotated at an even velocity by means of a motor 9. In the cylinder barrel, there is made a slot 10, parallel to the barrel circumference, at each outlet collar. Thus light is emitted onto the cuvette only when the slot corresponding to the cuvette in question is located at the respective outlet collar. The length of the slot, and the speed of rotation of the cylinder, are so matched that light is emitted onto the cuvette for the duration required by the measurement.
The slots 10 are located and prearranged on the cylinder barrel in succession, at even intervals, so that light is essentially transmitted to one cuvette at a time. This prevents the light scattered from the measuring beam of one cuvette from disturbing the measurement of another cuvette. Moreover, the slots are placed or pre-arranged so that successive emissions of light fall on cuvettes that are located as far as possible or spaced apart from each other (note the surface in FIG. 2). Thus successive measurements can, in order to save time, be somewhat overlapping (for instance about 10% of the measuring period of each cuvette) without remarkable errors being caused by scattered light. The time used in the measurement of one plate (transmissions included) is typically about 5.5 s.
Moreover, the surface of the cylinder is provided with holes 11 for each cuvette, these holes being placed in a straight row. The holes are meant to be used particularly in the measurement of agglutinations, in which case the measuring beam is allowed to scan over the bottom by moving the cuvette assembly.
Further, the cylinder comprises surface area 12 for defining the signal obtained from the detectors in cases where no light enters the cuvette.
The apparatus is synchronized so that when, after the measurement of one row 1 on the plate, the next row is shifted to the measuring position, the cylinder 8 makes one revolution.
In principle the measurement can can also be carried out without stopping the cuvette assembly. In that case, however, measuring accuracy is reduced owing to the vibration of the liquid surface.
Instead of a rotating cylinder, there can be employed a light-cutting rectangular disc or plate moving with respect to the cuvette assembly; or a light-cutting disc rotating underneath an immobile cuvette assembly, in which disc or plate the light-permeable slots are formed.